Spatially-spectrally swept optical memories and addressing methods

ABSTRACT

An optical data storage system directs a reference beam and a data beam to a storage material having an inhomogeneous linewidth. The data beam is modulated to contain data to be stored in the storage material. The reference beam and the data beam illuminate storage cells of the storage material, causing data to be stored. The reference beam and the data beam spatially scan the cells and are frequency swept during their respective spatial scans. Data is retrieved from the cells by illuminating the storage material with the reference beam to produce a reconstructed data beam. In an embodiment, the reference beam and the data beam overlap and illuminate the storage cells simultaneously. The reconstructed data beam is detected as a heterodyne signal produced by mixing the reconstructed data beam and the reference beam in a detector.

This application is a divisional of, and claims priority from, U.S.patent application Ser. No. 09/412,841, filed Oct. 5, 1999, now U.S.Pat. No. 6,618,342, which claims benefit of Provisional Application Ser.No. 60/103,001, filed Oct. 5, 1998.

TECHNICAL FIELD

The invention pertains to methods and apparatus for optical datastorage.

BACKGROUND

Optical data storage systems use changes in absorption, reflection,and/or refractive index of a storage material to store and retrievedata. In conventional optical data storage systems, individual spatiallocations (“cells”) on a substrate are allocated to store individualbits. A sequence of data bits is recorded in such memory systems bymapping each bit onto a different storage cell, and changing a materialparameter at each cell to represent the data bit. Readout of the memoryis accomplished by illuminating each cell with a light source. Inconventional implementations of such memories (CD-ROM, magneto-opticdisks, etc.), each cell records one data bit.

Rather than directly allocating each cell to an individual data bit,frequency-selective data storage (“FSDS”) memories have beendemonstrated in which multiple data bits are recorded in each storagecell. Volatile frequency-selective memories are disclosed in, forexample, U.S. Pat. No. 3,896,420, and non-volatile memories aredisclosed in, for example, U.S. Pat. No. 4,101,976. FSDS memories recordmultiple bits in each cell using materials that allow spectraladdressing of individual atoms or molecules. FSDS memories thus use bothspectral and spatial addressing to access different portions of thestorage material's absorption spectrum as well as different locations inthe storage material.

FSDS systems use storage materials that have inhomogeneously broadenedabsorption profiles such as the absorption profile 101 of FIG. 1. Anabsorption profile of an inhomogeneously broadened material (such as theabsorption profile 101) is characterized by an inhomogeneous linewidthΔν_(i) that is a measure of the spectral width of the absorption profile(typically the full width of the absorption profile at one-half of themaximum value of absorbance). The absorption profile results from asummation of absorption profiles from individual absorbers (atoms,molecules or other active absorber centers), each having a spectralabsorption profile and a spectral width referred to as a homogeneousabsorption profile and a homogeneous linewidth Δν_(h), respectively.FIG. 2 shows an example of a homogeneous absorption profile 201 of anindividual absorber. Inhomogeneous broadening arises from the differingmicroenvironments for individual absorbers shifting the opticalfrequencies at which absorption occurs. Thus, the inhomogeneousabsorption profile represents a combination of narrower, homogeneousabsorption profiles centered at different frequencies. FSDS systems usematerials in which the inhomogeneous linewidth is larger than thehomogeneous linewidth.

When an inhomogeneously broadened material is illuminated with a singlefrequency light source, only the absorbers resonant with this singlefrequency interact with the light, resulting in optical excitation ofthese absorbers. Illuminating such a material with light having abandwidth less than the material's inhomogeneous absorption linewidthproduces a dip, or “spectral hole” in the absorption profile. Theminimum width of a spectral hole is approximately equal to thehomogeneous absorption linewidth. FIG. 3 illustrates a spectral hole 301of width Δν_(h) in an inhomogeneous absorption profile 303. FSDS systemsuse multiple spectral holes to record multiple bits in a single cell.The number of spectral storage channels available in a single cell of aninhomogeneously broadened material is determined by the ratioΔν_(i)/Δν_(h) of the inhomogeneous linewidth Δν_(i) to the homogeneouslinewidth Δν_(h). The number of spectral channels used is referred to as“spectral multiplicity.” For additional discussion of spectralhole-burning, see, for example, W. E. Moerner, ed, Persistent SpectralHole Burning: Science and Applications (Springer Verlag, New York,1988).

Two types of FSDS systems have been demonstrated and both can achievethe same spectral multiplicity. The first type is referred to as“frequency-domain” FSDS, and the second class is referred to as“time-domain FSDS.” These two types are discussed briefly below. Inaddition to these two types of FSDS systems, a “swept-carrier” system isdisclosed in Mossberg, U.S. Pat. No. 5,276,637, incorporated herein byreference.

Frequency-domain FSDS systems directly address individual spectralchannels in an inhomogeneously broadened material. In such systems, anarrowband light source having a spectral width less than theinhomogeneous linewidth Δν_(i) illuminates a storage material. Acontinuous wave (“CW”) laser is typically used as the narrow-bandsource. Absorbers for which the narrow-band light source fulfills theresonant condition are excited, recording data. Photo-induced absorptionor refractive index changes produced by this excitation are probed toretrieve recorded data. If the linewidth Δν_(i) of the narrow-band lightsource is less than the homogeneous linewidth Δν_(h), the achievablestorage capacity in each cell is Δν_(i)Δν_(h). If the source linewidthΔν_(i) is larger than the homogeneous linewidth Δν_(h), then the storagecapacity is instead Δν_(i)/Δν_(i) and is said to be “laser linewidthlimited.”

Frequency-domain FSDS imposes data-rate limitations on single bitrecording. A spectral channel width Δν_(ch) must be addressed withillumination having a pulse duration greater than 1/Δν_(ch) because of aFourier-transform relationship between pulse duration and linewidth.Thus, to access the kHz-scale linewidths available in somerare-earth-doped crystals, recording and readout pulses of approximatelymillisecond durations are required. The spectral holes produced in suchFSDS systems can be either transient or permanent, as disclosed in U.S.Pat. No. 3,896,420, incorporated herein by reference.

Rather than allocating individual frequency channels to individual bits,time-domain FSDS systems use pulses with spectral widths larger than thehomogeneous linewidth Δν_(h) and therefore can use pulses with durationsless than 1/Δν_(h). Time-domain FSDS systems can record data streamscontaining pulses that are as short as 1/Δν_(i). In time-domain FSDSsystems, a storage material is exposed to a brief reference pulse and adata pulse corresponding to a data-bit stream. These pulses illuminatethe storage material sequentially to record an interference between thefrequency spectra of the reference pulse and the data pulse, resultingin the direct recording of the spectrum of the data-bit stream. If thereference pulse precedes the data pulse, subsequent illumination of thestorage material with a replica of the reference pulse produces areconstruction of the data pulse. Such time-domain FSDS systems aredescribed in, for example, U.S. Pat. No. 4,459,682, incorporated hereinby reference.

Time-domain FSDS systems use temporally distinct reference pulses torecord the spectrum of a data-bit stream, while swept-carrier FSDSsystems record the spectrum of a data-bit stream using frequency-swept(chirped) reference and data beams. The reference and data beamssimultaneously illuminate the storage material, and subsequentillumination with the frequency swept reference beam reproduces the databeam. Such systems are disclosed in, for example, Mossberg, U.S. Pat.No. 5,276,637 and Mossberg et al., Opt. Lett. 17, 535 (1992).

In conventional FSDS systems, a positioning system directs a laser beamto a particular cell, and data is recorded in, or read from, the entirespectral capacity at the cell. Thus, the laser is stationary in twospatial dimensions while the data is stored or retrieved using a thirddimension (frequency).

An important limitation of both time-domain and swept-carrier datastorage is excitation-induced frequency shifts, also referred to asexcitation-induced dephasing or instantaneous dephasing, as describedin, for example, Huang et al., Phys. Rev. Lett. 63, 78 (1989). Theexcitation-induced frequency shifts increase the homogeneous linewidthΔν_(h) with increasing levels of illumination. Thus, as data isrecorded, the data storage capacity of the material decreases. Thestorage capacity can be dramatically lower than the intrinsic storagecapacity. For example, in Eu³⁺-doped Y₂SiO₅, the intrinsic data storagecapacity based on the ratio of the inhomogeneous and homogeneouslinewidths is greater than 10⁶ bits/cell. See, for example, R. Equall etal, Phys. Rev. Lett. 72, 2179 (1994), Yano et al, J. Opt. Soc. Am. B 9,992 (1992). The storage capacity of Eu³⁺-Y₂SiO₅: drops to approximately2000 bits/cell whenever the inhomogeneous absorption profile of thestorage material is fully excited. Thus, while conventional time-domaindata-access methods provide fast data access, excitation-inducedfrequency shifts severely limit data-storage capacity.

SUMMARY OF THE INVENTION

Methods of storing data in cells of a storage material having aninhomogeneous absorption with an inhomogeneous linewidth Δν_(i), areprovided. The methods include directing a reference pulse ofelectromagnetic radiation and a data pulse of electromagnetic radiationto the storage material. The data pulse is modulated according to datato be stored in the cells of the storage material. The reference pulseand the data pulse are spatially-spectrally swept, causing data to bestored in the cells of the storage material. In some embodiments, thereference spatial-spectral trajectory and the data spatial-spectraltrajectory are the same while in other embodiments, the reference anddata spatial-spectral trajectories are offset in position or frequency.In a representative embodiment, the reference pulse and the data pulsesimultaneously illuminate each individual storage cell of the storagematerial and co-propagate to and through the storage material.

In a specific embodiment, a frequency sweep of at least one of thereference and data spatial-spectral trajectories is a linear sweep.

In other methods, a data bit is stored using a channel bandwidth Δν_(ch)and at least one of the spatial-spectral trajectories spans a frequencyrang that is larger than the channel bandwidth Δν_(ch).

Methods of storing a first data record and a second data record, thedata records including one or more data bits, include providing astorage material having an inhomogeneously broadened absorption oflinewidth (Δν_(i)) that is greater than the channel bandwidth (Δν_(ch))used to store a single data bit. A first reference pulse is providedthat has a first starting frequency within the inhomogeneous linewidth(Δν_(i)), a first starting spatial position on the storage material, andfollows a first spatial-spectral trajectory that spans a first spectralwidth greater than the channel bandwidth Δν_(ch). The channel bandwidthis less than or equal to the inhomogeneous linewidth Δν_(i). A firstdata pulse is also provided to the storage material. The first datapulse has a second starting frequency within the inhomogeneous linewidth(Δν_(i)) and a second starting spatial position on the storage material.The first data pulse follows a second spatial-spectral trajectory thatspans a second spectral width that is greater than the channel bandwidth(Δν_(ch)) and that is less than or equal to the inhomogeneous linewidth(Δν_(i)). The first data pulse has a modulation corresponding to a firstdata record. The first data record is stored in the storage material byexposing the storage material to the first data pulse and the firstreference pulse. A second reference pulse and a second data pulse areprovided, the second reference pulse and the second data pulse followinga third spatial-spectral trajectory and a fourth spatial-spectraltrajectory. These trajectories span spectral widths that are greaterthan the channel bandwidth (Δν_(ch)) and less than or equal to theinhomogeneous linewidth (Δν_(i)). Preferentially, the thirdspatial-spectral trajectory does not overlap the first spatial-spectraltrajectory but does overlap the fourth spectral-spatial trajectory. Thesecond data pulse has a modulation corresponding to a second data recordand the second data record is stored in the storage material by exposingthe storage material to the second reference pulse and the second datapulse.

In alternative embodiments, the storage material comprises multiplecells for storing portions of the first and second data sequences andthe multiple cells are exposed to the first reference pulse and thefirst data pulse simultaneously. In additional specific embodiments thestorage material is Eu³⁺:YSiO₅.

Apparatus for storing and retrieving data from a storage material havingan inhomogeneous absorption are provided. The apparatus comprise a laserthat produces a laser beam having a frequency that sweeps through afrequency range, a signal generator that generates a reference signal,and a data source that provides a data signal. A modulator such as anacousto-optic modulator, electro-optic modulator or other type ofmodulator receives the reference signal, the data signal, and the laserbeam and generates a reference beam and a data beam. The data beam ismodulated by the data signal, and the data beam and the reference beamare co-propagating. A scanner scans the data beam and the reference beamacross the storage material, so as to cause data to be stored in cellsof the storage material. A detector is provided that receives thereference beam transmitted by a cell and a reconstructed data beamproduced by the transmission of the reference beam through the cell. Thedetector producing a heterodyne signal from the reference andreconstructed data beams, wherein the heterodyne signal has a modulationcorresponding to data retrieved from the storage material.

These and other features of the invention are set out below withreference to the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates an inhomogeneous absorption profile of afrequency-selective material having an inhomogeneous linewidth Δν_(i).

FIG. 2 illustrates a homogeneous absorption profile of a singlerepresentative absorber of a frequency-selective material, theabsorption profile having a homogeneous linewidth Δν_(h).

FIG. 3 illustrates a spectral hole burned in the inhomogeneousabsorption profile of FIG. 1.

FIG. 4 is a block diagram of a swept spatial-spectral memory system.

FIG. 5 illustrates four spatial-spectral trajectories swept by thesystem of FIG. 4.

FIG. 6 illustrates a specific embodiment of a system for optical datastorage and retrieval.

FIG. 7 illustrates four representative spatial-spectral trajectoriesobtained with the system of FIG. 6.

FIGS. 8A-8D illustrate data retrieved using the system of FIG. 6 atdifferent swept rates.

DETAILED DESCRIPTION

The following terms are used herein:

Co-propagating: Beams that propagate in a common direction and thatspatially overlap are co-propagating beams.

Data wave: Electromagnetic radiation used to record data or a datasequence, and having a modulation corresponding to the data or datasequence. Also referred to as a “data beam” or a “data pulse.” As usedherein, electromagnetic radiation or optical radiation refers toelectromagnetic radiation at a frequency matched to the inhomogeneousabsorption profile of a selected storage material.

FSDS: “Frequency-selective data storage,” i.e., recording data in afrequency-selective material using spectral multiplexing by storingdifferent data in different portions of an inhomogeneous absorptionprofile. FSDS includes frequency-domain, time-domain, and swept-carrierdata storage.

Direct-detection swept-carrier data storage: Swept-carrier FSDS in whichthe reference and data waves are not co-propagating. The reference anddata waves spatially overlap at the storage material (but generally notat other positions) producing a reconstructed data wave that is areplica of the data wave.

Spatial-spectral Sweep: A variation of frequency and position of a wave.A spatial-spectral sweep defines an area in space-frequency coordinatesreferred to as a “trajectory.”

f_(m): A frequency range spanned by a spatial-spectral sweep.

Heterodyne swept-carrier data storage: Swept-carrier FSDS in which thereference and data waves are co-propagating and the data is recovered asa heterodyne beat frequency between the transmitted reference wave andthe reconstructed data wave.

Homogeneous linewidth, Δν_(h): The linewidth of a single absorptioncenter.

Inhomogeneous linewidth a Δν_(i): The collective linewidth of a multipleabsorbers in a unit of storage material having a distribution of center(resonance) frequencies.

Intrinsic capacity: The maximum storage capacity of an FSDS material,generally expressed by the ratio Δν_(i)/Δν_(h) and neglectingexcitation-dependent line broadening.

Reference wave: One of two waves used to record a data sequence. Duringrecording, the reference wave is used to prepare the storage material.After data is recorded, illumination with the reference wave produces areconstructed data wave that corresponds to the data wave.

Spotlet: A region at the storage material illuminated by a data wave orother wave at any one instant. A spotlet is also referred to as a “beamdiameter” and corresponds to a beam waist or beam spot size.

Superspot: A region of the storage material illuminated by spatiallysweeping the recording waves (the data wave and the reference wave) orthe wave used to reconstruct data (the reference wave). A superspot is aset of spotlets.

T_(sweep): A time required to store or retrieve data in aspatial-spectral sweep of a superspot.

τ_(b): The duration of a single bit in a data sequence.

X_(m): A spatial range spanned in a spatial-spectral sweep. In someexamples, X_(m) is a spatial extent of a superspot.

X_(sp): A spatial diameter of a spotlet.

Δν_(ch): Channel bandwidth. The spectral width of an inhomogeneousabsorption line allocated to the storage of a single bit.

Methods are provided for simultaneous spectral and spatial access to afrequency-selective optical storage material. These methods improve theperformance of FSDS systems, by, for example, reducing the effects ofexcitation-induced frequency shifts. In the storage methods and systemsdisclosed herein, an optical reference beam (or pulse) and an opticaldata beam (or pulse) are simultaneously swept across a storage materialwhile the respective beam frequencies are changed.

Absorbers in the storage material can be described with reference to aposition-frequency coordinate system having coordinate axes thatrepresent the spatial coordinates of each absorber and a spectralcoordinate that represents each absorbers' position within aninhomogeneous absorption profile. In a representative embodiment, datais stored and retrieved using laser beams that follow predeterminedtrajectories in position-frequency space. During a particular read orwrite operation, different portions of the available inhomogeneousabsorption profile are typically accessed at different spatial locationsof the storage material. Since excitation at one spatial location doesnot contribute strongly to excitation-induced frequency shifts atadjacent spatial locations, the net effect of excitation-inducedfrequency shifts is reduced. The entire position-frequency space volumeof the storage material can be used for data storage with multiplestorage and retrieval operations.

Such systems use simultaneous spatial and spectral scanning during thedata-recording and data-retrieval processes. Spatial-spectral scanningproduces a path or trajectory in position-frequency space, referred toherein as a “spatial-spectral trajectory.” The spatial-spectraltrajectories can be individually varied to optimize performance forvarious storage material properties and to reduce excitation-inducedline broadening.

FIG. 4 illustrates a spatial-spectral sweep apparatus 5. The apparatus 5includes a narrow-band, continuous wave, tunable laser 10 that producesa laser beam 20 at a wavelength suitable for the excitation of a storagematerial 16 having an inhomogeneous absorption profile. A frequencyscanner 11 tunes the laser 10, sweeping the wavelength of the laser beam20 across the inhomogeneous absorption profile of the storage material16. A shutter 12 blocks the laser beam 20 whenever data is being neitherrecorded in nor retrieved from the storage material 16.

A modulation system 13 transmits the laser beam 20 and produces areference beam 21 and data beam 23. Data to be recorded in the storagematerial 16 are modulated onto the data beam 23. The reference beam 21and the data beam are received by a spatial address system 14 that issituated to angularly deflect the reference beam 21 and the data beam23. An optical delivery system 15 converts the angular deflectionsproduced by the spatial address system 14 into corresponding spatialdisplacements of the reference beam 21 and the data beam 23, and directsthe spatially displaced beams to the storage material 16. Aftertransmission through the storage material 16, an optical collectionsystem 17 directs the transmitted data and reference beams to an opticaldetector 18 that is used for data retrieval. A detector signal 27 fromthe optical detector 18 is delivered to a processing system 25 thatproduces a signal corresponding to the retrieved data. The processingsystem is in communication with a control system 19 that controls thefrequency scanner 11, the shutter 12, the modulator system 13, thespatial address system 14, and the optical detector 18. The detector 18is generally active only during data retrieval and is unnecessary duringdata storage.

In an example of data storage, the frequency range used by each data bitto be stored is approximately τ_(b) ⁻¹, where τ_(b) is a duration of thedata bit. To store a spectral interference between the reference beamand the data beam, the laser beam 20 preferably has a coherence timelonger than about T_(sweep)/(f_(m)τ_(b)) or 1/τ_(b), whichever islonger, wherein T_(sweep) is a time duration used to sweep the frequencyof the reference beam 21 or the data beam 23 over a frequency rangef_(m). The frequency scanner 11 controls the frequency of the laser 10,thereby tuning the laser 10 over a frequency range f_(m) in a timeduration T_(sweep). To fully use the spectral bandwidth of the storagematerial 16, the frequency range f_(m) is greater than or equal to theinhomogeneous linewidth Δν_(i). The time duration T_(sweep) is selectedto provide a selected combination of bit rate and storage capacity,wherein T_(sweep)=τ_(b) N_(b) and N_(b) is a number of bits.

In FIG. 4, the shutter 12 is shown as a separate component, but theshutter 12 can be included in the modulation system 13.

The modulation system 13 produces both the data beam 23 (a data wave)that is modulated by a data signal and the reference beam 21. Thereference beam 21 and the data beam 23 can be offset in frequencyrelative to each other and can be either co-propagating or spatiallyseparate. In an example, the frequency offset between the reference waveand the data wave is (2τ_(b))⁻¹. In the system 5 of FIG. 4, the databeam 23 and the reference beam 21 use a common frequency sweep appliedto the laser 10, but the beams can be individually swept over differentrespective frequency ranges.

The spatial addressing system 14 directs the reference and data beamsfrom the modulation system 13 into varying spatial directions. Thenumber of distinguishable spatial directions (angles or beam diameters)obtainable using the spatial address system 14 determines acorresponding number of independently addressable spots in the storagematerial 16. The number of distinguishable spatial directions dependsupon the range of deflection angles produced by the spatial addresssystem 14 and the diffraction angle of the laser beam 20.

The optical delivery system 15 directs the reference and data beams tothe storage material 16 and focuses the reference and data beams on thestorage material 16. The optical delivery system 15 overlaps the commonfrequency components of the two waves at the storage material 16. Thesize of each of the focused spots is selected to maximize anoutput-signal magnitude obtainable during data retrieval and to fullyuse all of the available cells of the storage material 16. The beam spotsize at the storage material 16 is referred to herein as a “spotletsize” (t_(sp)).

The storage material 16 is selected to have properties suited to a givenapplication, based on material properties such as intrinsic capacity (aratio of Δν_(i)/Δν_(h)) and data storage time. An example material isEu³⁺-doped Y₂SiO₅, having an intrinsic capacity of greater than 10⁶bits/cell, and a data storage time of hours. This material isappropriate for high-density, dynamic optical memories and is describedin, for example, R. Equall et al., Phys. Rev. Lett. 72, 2179 (1994) andYano et al., J. Opt. Soc. Am. B 9, 992 (1992), both of which areincorporated herein by reference. Another suitable storage material isany of a various Tm³⁻doped inorganic crystals that provide storagematerials having intrinsic capacities of 10⁶ bits/spot and storage timesof up to 10 ms. Consequently, such Tm³⁺-doped materials are appropriatefor use in buffer memories. These materials are discussed in, forexample, Macfarlane, Opt. Lett. 18, 829 (1993).

The optical collection system 17 collects a “reconstructed data beam”from the storage material 16 and directs the reconstructed data beam aswell as a reference beam onto the detector 18. In order to recover thestored data, the detector has a bandwidth greater than τ_(b) ⁻¹. Inaddition, the detector desirably has a sensitivity sufficient for thedetection of the reconstructed data beam.

The spatial-spectral sweep apparatus 5 of FIG. 4 operates as follows. Tostore a set of data within a single superspot, the laser 10 is tuned bythe frequency scanner 11 to a first frequency, the spatial addresssystem 14 selects a first spatial location (cell) on the storagematerial 16 for storing the data, and the shutter 12 opens to allow thereference beam 21 and the data beam 23 to pass through. During datastorage, a linear or nonlinear ramp is applied to the frequency scanner11 and to the spatial address system 14, generating spatial and spectraltrajectories (sweeps). As the frequency of the laser 10 is scanned, datais modulated onto the data beam by the modulation system 13. Severalrepresentative spatial-spectral trajectories 503, 504, 505, 506 areshown in FIG. 5. Starting points of adjacent trajectories are displacedin space or frequency in the figure. The output frequency of the laser10 is swept over the frequency range f_(m) and a spatial range X_(m),and the respective time-dependent spectra of the beams are stored in thestorage material 16. Referring to FIG. 5, in a first frequency sweep,data is stored along the trajectory 503. After the sw ep of thetrajectory 503 is complete, a second sweep, beginning at the frequencyf_(o), stores data along the trajectory 504. Data is stored alongtrajectories 505, 506 in additional sweeps that are similarly displaced.During quiescent periods between trajectories and following the storageof the last trajectory, the shutter 12 is closed.

The spatial-spectral sweep apparatus 5 spatially spreads a data-bitsequence across positions and frequencies specified by the sweeptrajectories. Although FIG. 5 shows linear trajectories, non-linearspatial and spectral trajectories can be used. In addition, the spatialand spectral sweeps need not be linear functions of time.

To retrieve a stored data sequence, the frequency and position of thelaser 10 are reset to initial values. The shutter 12 is opened and thespatial-spectral sweep used for data storage is repeated using only thereference beam 21. During data retrieval, the reference beam 21interacts with the storage material 16 and produces a reconstructed databeam corresponding to the original data beam 23. The reconstructed databeam is collected by the collection system 17, directed to the detector18, and converted back into an electronic data sequence, correspondingto the stored data sequence, by the processing system 25.

The apparatus 5 of FIG. 4 increases the storage capacity ofswept-carrier FSDS systems by illuminating only a small portion of theinhomogeneous absorption profile in a spatial cell at any one instant.Some storage materials include absorbers that can be considered asthree-level systems having a ground state, an excited state, and a trapstate. Excitation by an absorber causes a transition from the groundstate to the excited state. The excited state decays to the trap state,and the trap state eventually decays to the ground state, typically witha time constant in the range of a tens of milliseconds to hours. Theexcited state decays much more rapidly to the trap state with a timeconstant referred to as an “excitation lifetime.” To avoidexcitation-induced storage-capacity reductions, a spatial cell should beilluminated only a few times (preferably only once) during a timeinterval equal to or approximately equal to the excitation lifetime.After an absorber has relaxed to the trap state, the absorber no longercontributes significantly to excitation-induced line broadening. Inaddition, the data beam and the reference beam need not be appliedsimultaneously but within a dephasing time T₂ that is corresponds to aduration required for the phase of the excited state to be randomized.

To fully use the inhomogeneous absorption profile, the recordedsuperspots desirably partially overlap spatially. For example, thespatial-spectral trajectories 503-505 of FIG. 5 partially overlap eachother at a position at which X=X_(o), but there is no spectral overlapat such locations. Although the spatial sweep is generallytwo-dimensional, for convenience the trajectories 503-506 showone-dimensional sweeps.

As shown in FIG. 5, the spatial-spectral trajectories 503-506 arelinear. As the laser 10 is swept along a spatial-spectral trajectory,each cell receives an excitation over specific spectral bandwidths fromthe reference and data beams. For accurate data retrieval, theexcitation bandwidths experienced by a cell from the reference beam andth data beam are approximately equal. If τ_(b) ⁻¹>f_(m)τ_(b)/T_(sweep),then the number of spotlets N in each superspot preferably satisfies thecondition N<f_(m)τ_(b). Since excitation-induced broadening of Δν_(h)produced by increasing illumination of the storage material 16 isapproximately linear with the magnitude of the received excitation, andbecause the capacity of a frequency-selective storage material isinversely proportional to Δν_(h), the storage capacity of an FSDS systemcan be increased by a factor of about N using a spatial-spectral sweepaccording to the invention.

FIG. 6 shows a specific example of a spatial-spectral sweep apparatus601 using collinearly propagating data and reference beams. A modulator603 sinusoidally modulates a ring dye laser 605, producing a laser beam607 that sweeps repetitively over a 1 GHz frequency range with a 6.25 msperiod. During data storage, a reference signal 609 and a data signal611, supplied by a reference generator 613 and a data source 615,respectively, are applied to an acousto-optic modulator 616 to produce areference beam 617 and a data beam 619, respectively. The reference beam617 and the data beam 619 have a frequency offset of 4 MHz, and the databeam 619 is amplitude-modulated with binary data to be stored in astorage material 620. With this frequency offset, the reference beam 617and the data beam 619 are collinear within a diffraction limit of thebeams 617, 619. During data retrieval, a read signal is applied to theacousto-optic modulator 616 to generate a reconstructed data beam 641.

A modulator 621 drives an acousto-optic deflector 623 synchronously withthe laser frequency sweep and deflects the co-propagating reference beam617 and data beam 619. A lens 627 receives the both beams and focusesthe beams to a selected storage location in the storage material 620. Inthis embodiment, the storage material 620 is a 10 mm by 11 mm by 2 mmEu³⁺:Y₂SiO₅ crystal that is maintained at a temperature of about 5 K ina flowing helium cryostat 631. The combined beams propagate along abaxis (the 2 mm direction) of the Eu³⁺:Y₂SiO₅ crystal and are polarizedalong a D₁-axis. Peak powers in the data, reference, and reconstructeddata beams are all about 300 μW and the spot size of each of the beamsis about 40 μm.

Data stored in the storage material 620 is retrieved by directing areference beam to the storage material 620 to generate the reconstructeddata beam 641 corresponding to the data beam 619. The reconstructed databeam 641 and the reference beam are then focused by a lens 633 onto adetector 635 to produce a heterodyne beat signal at a data-referencebeam offset frequency of 4 MHz. This heterodyne signal is electronicallyprocessed by a receiver module 637 to produce an electrical signal thatcorresponds to the stored data. In this example, the reference beamserves as a local oscillator for the reconstructed data wave.

FIG. 6 illustrates a spatial-spectral sweep apparatus 601 that producesa heterodyne signal during data retrieval, i.e., carrier frequencies ofthe reference beam and the reconstructed data beam are not equal).Similar apparatus are possible that mix an external local oscillator(instead of a portion of the reference signal) with a reconstructed databeam to produce a homodyne signal. Alternatively, a portion of theunmodulated data beam can be transmitted to serve as a local oscillator.

FIG. 7 illustrates spatial-spectral trajectories 703-707 swept by thesystem 601 of FIG. 6. Each of the trajectories 703-707 includes arespective spectral sweep over a frequency range f_(m) and a spatialsweep over a spatial range X having a spotlet size d. Because the periodof the frequency scan produced by the acousto-optic modulator 616 is6.25 ms, scanning the five trajectories 703-707 requires a minimum of31.25 ms. In other embodiments, the time interval can be longer orshorter.

FIGS. 8A-8D show examples of stored data retrieved during a 300 μs timeinterval during data retrieval. The data correspond to data stored in atrajectory area 709 shown in FIG. 7, but the retrieved data of FIGS.8A-8D were obtained without storing data along the trajectories 703,705-707.

In FIGS. 8A-8D, the respective retrieved data bits are shown asrespective magnitudes (on an arbitrary scale) as a function of time atwhich each bit is retrieved. FIGS. 8A-8D represent data retrieval withrespective spatial scan ranges (X-values) of 0 μm, 36 μm, 160 μm, and440 μm, corresponding to average sweep rates of 0 μm/ms, 120 μm/ms, 530μm/ms, and 1550 μm/ms, respectively. FIG. 8A shows that with no sweep,only a few data bits are retrieved and that these data bits areretrieved with small magnitudes. FIGS. 8B-8D demonstrate that moreextensive spatial sweeps permit better retrieval of larger numbers ofdata bits. Sweep rates are generally selected to that any spatial cellreceives approximately the same spectral bandwidth from both the databeam and the reference beam, i.e., the sweep rate is selected so that aproduct of a frequency sweep rate R_(sweep) and an exposure time Δt_(b)is approximately equal to a bit bandwidth Δτ_(b). The sweep rate is alsoselected based on illumination intensity to achieve a selected productof illumination intensity and exposure time.

The embodiment described above is illustrative, and the scope of theinvention is not to be constrained by the specific details presentedtherein. The invention rather should be understood to include a generalclass of devices that use the methods described and of which the aboveembodiments are particular examples. The particular values chosen forparameters such as reference beam/data beam frequency offset, number ofspotlets, etc, correspond to a particular choice of values for aparticular implementation, and the invention is not restricted to thedisclosed values.

Although a tunable laser is used in the embodiments discussed above anarrow-band, fixed-frequency laser can alternatively be used, whereinthe frequency sweep produced external to the laser, using, for example,an acousto-optic or electro-optic modulator.

In the embodiment of FIG. 4, the spatial address system 14 is used toaddress spatial locations on the storage material 16. Alternatively, thestorage material 16 can be moved physically to produce aspatial-spectral sweep. Such spatial-spectral addressing would beparticularly well suited to a disk-based optical memory.

The system 5 of FIG. 4 uses data and reference beams that propagate andare deflected together. In alternative systems, the data and referencebeams overlap only at the storage material. As such alternative systemsare constrained by excitation-induced frequency shifts in the samemanner as the system of FIG. 4, the spatial-spectral sweep methoddisclosed herein is also of benefit to systems that do not useco-propagating beams.

The wavelengths or the reference beam and the data beam can be selectedbased on the inhomogeneous absorption profile of the storage materialand includes visible light as well as other wavelengths that areresonant with at particular inhomogeneous absorption profile.

The invention is directed to novel and non-obvious aspects of thisdisclosure, both individually and in combination as set forth in theclaims below. While the invention is described with respect toparticular implementations, the invention is not limited to theseimplementations.

1. An apparatus for storing and retrieving data from a storage materialhaving an inhomogeneous absorption, comprising: a laser that produces alaser beam having a frequency that sweeps through a frequency range; asignal generator that generates a reference signal; a data source thatprovides a data signal; an acousto-optic modulator that receives thereference signal, the data signal, and the laser beam and generates areference beam and a data beam, the data beam modulated by the datasignal, wherein the data beam and the reference beam are co-propagating;a scanner that scans the data beam and the reference beam across thestorage material, so as to cause data to be stored in cells of thestorage material; and a detector situated to recieve the reference beamtransmitted by a cell and a reconstructed data beam produced bytranmission of the reference beam through the cell, the detectorproducing a heterodyne signal from the reference and reconstructed databeams, wherein the heterodyne signal has a modulation corresponding todata retrieved from the storage material.
 2. The apparatus of claim 1,wherein the storage material is Eu³⁺:YSiO₅.